Classical electrodynamicsThis edition refines and improves the first edition. It treats the present experimental limits on the mass of photon and the status of linear superposition, and introduces many other innovations. 
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Page 75
The edges of the box shown in Fig. 2.9 are one example, the corners at x = 0, y=0
and x = a, y = 0 in Fig. 2.10 another. It is useful therefore to have an
understanding of how the potential, the fields, and the surface charge densities
behave in ...
The edges of the box shown in Fig. 2.9 are one example, the corners at x = 0, y=0
and x = a, y = 0 in Fig. 2.10 another. It is useful therefore to have an
understanding of how the potential, the fields, and the surface charge densities
behave in ...
Page 389
8.12 Discuss the reflection by a flat strip of width d, centered at x = x<>, in a
rectangular guide, as shown in Fig. 8.15. (a) Use the approximation of K(x) = 1 in
(8.156) to show that the shunt impedance is approximated by (b) For a centered
strip ...
8.12 Discuss the reflection by a flat strip of width d, centered at x = x<>, in a
rectangular guide, as shown in Fig. 8.15. (a) Use the approximation of K(x) = 1 in
(8.156) to show that the shunt impedance is approximated by (b) For a centered
strip ...
Page 482
The first instability is the kink instability, shown in Fig. 10.6a. The lines of
azimuthal magnetic induction near the column are bunched together above, and
separated below, the column by the distortion downwards. Thus the magnetic
pressure ...
The first instability is the kink instability, shown in Fig. 10.6a. The lines of
azimuthal magnetic induction near the column are bunched together above, and
separated below, the column by the distortion downwards. Thus the magnetic
pressure ...
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Contents
Introduction and Survey  1 
Introduction to Electrostatics  27 
BoundaryValue Problems  54 
Copyright  
18 other sections not shown
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4vector amplitude angle angular distribution angular momentum aperture approximation assumed atomic axis behavior Bessel functions boundary conditions bremsstrahlung calculation Chapter charge density charge q charged particle classical coefficients collision components conductor consider coordinates cross section current density cylinder defined dielectric constant differential diffraction dimensions dipole direction discussed effects electric and magnetic electric field electromagnetic fields electrons electrostatic energy loss expansion expression factor finite force frequency given Green function incident integral Lagrangian limit linear Lorentz transformation macroscopic magnetic field magnetic induction magnitude Maxwell equations medium modes molecules multipole multipole expansion multipole moments nonrelativistic normal obtain oscillations parallel parameter photon Phys plane wave plasma point charge polarization problem propagation quantum quantummechanical radius region relativistic resonant rest frame result scalar scalar potential scattering shown in Fig solution spectrum sphere spherical surface tensor theorem transverse unit vanishes vector potential velocity wave guide wave number wavelength written zero